Search results for "nuclear physics"

showing 10 items of 5307 documents

Measurement of the relative branching fractions ofB¯→D/D*/D**l−ν¯ldecays in events with a fully reconstructedBmeson

2007

We determine the relative branching fractions of semileptonic B decays to charmed final states. The measurement is performed on the recoil from a fully reconstructed B meson in a sample of 362×106 BB pairs collected at the Υ(4S) resonance with the BABAR detector. A simultaneous fit to a set of discriminating variables is performed on a sample of B→DX-ν decays to determine the contributions from the different channels. We measure Γ(B-→D-ν)/Γ(B-→DX-ν)=0.227±0. 014±0.016, Γ(B-→D*-ν)/Γ(B-→DX- ν)=0.582±0.018±0.030, and Γ(B-→D **-ν)/Γ(B-→DX-ν)=0.191±0. 013±0.019 for the charged B sample, and Γ(B0→D- ν)/Γ(B0→DX-ν)=0.215±0.016±0. 013, Γ(B0→D*-ν)/Γ(B0→DX- ν)=0.537±0.031±0.036, and Γ(B0→ D**-ν)/Γ(B0→…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionResonance01 natural sciencesParticle identificationXi baryonNuclear physicsParticle decayRecoil0103 physical sciencesB meson010306 general physicsPhysical Review D
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Measurement of the shape of the boson rapidity distribution forpp¯→Z/γ*→e+e−+Xevents produced atsof 1.96 TeV

2007

We present a measurement of the shape of the boson rapidity distribution for p (p) over bar -> Z/gamma(*)-> e(+)e(-)+X events at a center-of-mass energy of 1.96 TeV. The measurement is made for events with electron-positron mass 71 < M-ee < 111 GeV and uses 0.4 fb(-1) of data collected at the Fermilab Tevatron collider with the D0 detector. This measurement significantly reduces the uncertainties on the rapidity distribution in the forward region compared with previous measurements. Predictions of next-to-next-to-leading order (NNLO) QCD are found to agree well with the data over the full rapidity range.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsTevatron7. Clean energy01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesRange (statistics)High Energy Physics::ExperimentRapidityFermilab010306 general physicsColliderBosonBar (unit)Physical Review D
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Medium-modified jets and initial state fluctuations as sources of charge correlations measured at energies available at the BNL Relativistic Heavy Io…

2011

We investigate the contribution of medium-modified jets and initial state fluctuations to the asymmetry in charged-particle production with respect to the reaction plane. This asymmetry has been suggested as a compelling signature for the chiral magnetic effect in QCD and makes the study of conventional scenarios for the creation of such charged-particle multiplicity fluctuations a timely endeavor. The different path-length combinations of jets through the medium in noncentral heavy ion collisions result in finite correlations of like and different charged particles emitted in the different hemispheres. Our calculation is based on the combination of jet events from Yet another Jet Energy-Lo…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsmedia_common.quotation_subjectElliptic flowObservable7. Clean energy01 natural sciencesAsymmetryCharged particleNuclear physicsParticle decay0103 physical sciencesQuark–gluon plasma010306 general physicsRelativistic Heavy Ion Collidermedia_commonPhysical Review C
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Top-pair forward-backward asymmetry beyond next-to-leading order

2011

We make use of recent results in effective theory and higher-order perturbative calculations to improve the theoretical predictions of the QCD contribution to the top-quark pair production forward-backward asymmetry at the Tevatron. In particular, we supplement the fixed-order next-to-leading order calculation with higher-order corrections from soft-gluon resummation at next-to next-to-leading order accuracy performed in two different kinematic schemes, which allows us to make improved predictions for the asymmetry in the $p\overline{p}$ and $t\overline{t}$ rest frames as a function of the rapidity and invariant mass of the $t\overline{t}$ pair. Furthermore, we provide binned results which …

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physics530 Physics010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyOrder (ring theory)01 natural sciencesAsymmetryGluonNuclear physicsPair production10231 Institute for Computational Science0103 physical sciencesHigh Energy Physics::ExperimentRapidityInvariant mass3106 Nuclear and High Energy Physics3101 Physics and Astronomy (miscellaneous)Resummation010306 general physicsmedia_commonPhysical Review D
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Exclusive production of pion and kaon meson pairs in two photon collisions at LEP

2003

Exclusive production of pi and K meson pairs in two photon collisions is measured with ALEPH data collected between 1992 and 2000. Cross-sections are presented as a function of cos theta* and invariant mass, for \ cos theta* \ < 0.6 and invariant masses between 2.0 and 6.0 GeV/c(2) (2.25 and 4.0 GeV/c(2)) for pions (kaons). The shape of the distributions are found to be well described by QCD predictions but the data have a significantly higher normalization. (C) 2003 Published by Elsevier B.V.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsAlephMeson010308 nuclear & particles physicsHigh Energy Physics::LatticeInvariant (physics)16. Peace & justice01 natural sciencesNuclear physicsAngular distributionPion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Mass spectrumHigh Energy Physics::ExperimentInvariant massNuclear Experiment010306 general physicsParticle Physics - ExperimentPhysics Letters B
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Charged particle multiplicity in e^{+}e_{-}$ → q[L:q] events at 161 and 172 GeV and from the decay of the W boson

1998

The data collected by DELPHI in 1996 have been used to measure the average charged particle multiplicities and dispersions in $q\bar{q}$ events at centre-of-mass energies of $\sqrt{s}=161$~GeV and $\sqrt{s}=172$~GeV, and the average charge multiplicity in WW events at $\sqrt{s}=172$~GeV. The multiplicities in $q\bar{q}$ events are consistent with the evolution predicted by QCD. The dispersions in the multiplicity distributions are consistent with Koba-Nielsen-Olesen (KNO) scaling. The average multiplicity of charged particles in hadronic W decays has been measured for the first time; its value, $19.23 \pm 0.74 (stat+syst)$, is consistent with that expected for an $e^+e^-$ interaction at a c…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsAnnihilation010308 nuclear & particles physicsElectron–positron annihilationHadronMultiplicity (mathematics)PartonCharge (physics)01 natural sciencesCharged particleNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysics letters: B
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Ds+ meson production at central rapidity in proton–proton collisions at s=7 TeV

2012

The pt-differential inclusive production cross section of the prompt charm-strange meson D_s in the rapidity range |y| phi pi, with phi -> KK, and its charge conjugate, about 480 D_s mesons were counted, after selection cuts, in the transverse momentum range 2

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsAntiparticleLarge Hadron ColliderMeson010308 nuclear & particles physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyHadronElementary particle7. Clean energy01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsLeptonPhysics Letters B
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Results on longitudinal spin physics at COMPASS

2016

Abstract The COMPASS experiment at the CERN SPS has taken data for deep inelastic scattering of polarised muons off a polarised NH3 target in 2007 and 2011 and off a polarised 6LiD target in 2002–2004 and 2006. We present our new results on the longitudinal double spin asymmetry A 1 p and the spin-dependent structure function g 1 p obtained from the 2011 data set. These results are used in a NLO QCD fit to the world data to obtain the polarised parton distributions. Also an update on our results on the Bjorken sum rule, connecting the integral of the non-singlet spin-dependent structure function with the ratio of the weak coupling constants, is given. The gluon polarisation can be accessed …

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsComputer science010308 nuclear & particles physicsPhysicsQC1-999High Energy Physics::PhenomenologyHadronPartonDeep inelastic scatteringEngineering physics01 natural sciencesGluonNuclear physicsCompass0103 physical sciencesCOMPASS experimentHigh Energy Physics::ExperimentSum rule in quantum mechanicsNuclear Experiment010306 general physicsParticle Physics - ExperimentNuclear and Particle Physics Proceedings
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The b-quark mass from non-perturbative Nf=2 Heavy Quark Effective Theory at O(1/mh)

2014

Abstract We report our final estimate of the b-quark mass from N f = 2 lattice QCD simulations using Heavy Quark Effective Theory non-perturbatively matched to QCD at O ( 1 / m h ) . Treating systematic and statistical errors in a conservative manner, we obtain m ¯ b MS ¯ ( 2 GeV ) = 4.88 ( 15 ) GeV after an extrapolation to the physical point.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsConservation lawHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyLattice field theoryExtrapolationLattice QCDBottom quarkNuclear physicsHeavy quark effective theoryHigh Energy Physics::ExperimentNon-perturbativePhysics Letters B
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Measurement of the strong coupling constant alfa_s from global event-shape variables of hadronic Z decays

1991

Abstract An analysis of global event-shape variables has been carried out for the reaction e+e−→Z0→hadrons to measure the strong coupling constant αs. This study is based on 52 720 hadronic events obtained in 1989/90 with the ALEPH detector at the LEP collider at energies near the peak of the Z-resonance. In order to determine αs, second order QCD predictions modified by effects of perturbative higher orders and hadronization were fitted to the experimental distributions of event-shape variables. From a detailed analysis of the theoretical uncertainties we find that this approach is best justified for the differential two-jet rate, from which we obtain αs(MZ2) = 0.121 ± 0.002(stat.)±0.003(s…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsElectron–positron annihilationHadronMeasure (mathematics)Hadronizationlaw.inventionNuclear physicsRenormalizationlawHigh Energy Physics::ExperimentColliderConstant (mathematics)Particle Physics - Experiment
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